Showing posts with label #95. Show all posts
Showing posts with label #95. Show all posts
Nuclear & Particle Physics – Scattering cross section
A beam of 1012 protons per second is incident on a target containing 1020 nuclei per square cm. At an angle of 10 degrees, there are 102 protons per second elastically scattered into a detector that subtends a solid angle of 10−4 steradians. What is the differential elastic scattering cross section, in units of sq cm per steradian?
A. 1024
B. 1025
C. 1026
D. 1027
E. 1028
(GR9277 #95)
Solution:
Using dimension analysis:
the fractional scattering rate:
In units of sq cm per steradian:
Answer: C
Thermal Physics - Carnot Cycle
In the cycle shown above, KL and NM represent isotherms, while KN and LM represent reversible adiabats. A system is carried through the Carnot cycle KLMN, taking in heat Q2 from the hot reservoir T2 and releasing heat Q1 to the cold reservoir T1. All of the following statements are true, EXCEPT:
A. Q1/T1 = Q2/T2
B. The entropy of the hot reservoir decreases
C. The entropy of the system increases
D. The work
E. The efficiency of the cycle is independent of the working substance.
(GR8677 #95)
Solution:Carnot engine efficiency:
where W = Q2 − Q1 → work done
(D) TRUE
The efficiency η does not depend on the working substance
(E) TRUE
W = Q2 − Q1
η = (Q2 − Q1)/Q2 = 1 − (Q1/Q2) = 1 − (T1/T2)
Q1/Q2 = T1/T2
Q1/T1 = Q2/T2
(A) TRUE
The hot reservoir has decreasing entropy because it gets cooler as the cycle proceeds.
(B) TRUE
In order to approach the Carnot efficiency, the processes involved in the heat engine cycle must be reversible and involve no change in entropy.
(C) FALSE
Answer: C
Electromagnetism – Dielectric
An infinite slab of insulating material with dielectric constant K and permittivity ɛ = Kɛ0 is placed in a uniform electric field of magnitude E0. The field is perpendicular to the surface of the material. The magnitude of the electric field inside the material is
B. E0/Kɛ0
C. E0
D. Kɛ0E0
E. KE0
(GR0177 #95)
Solution:In vacuum, E0 = σ/ɛ0
In dielectric, E = σ/ɛ
where ɛ = Kɛ0
Thus, E = σ/Kɛ0 = E0/K
Answer: A
Quantum Mechanics - Commutation Relations
Let
be a quantum mechanical angular momentum operator. The commutator [
,
] is equivalent to which of the following?
A. 0
B. iħ
C. iħ

D. −iħ

E. iħ

Commutator identities: [A, B] = − [B, A]
and, [B, AC] = A[B, C] + [B, A]C
[
,
] = − [
, 
]
A =
B =
C =
[
, 
] =
[
,
] + [
,
]
=
[
,
] + 0
=
[iħ
] + 0
− [
, 
] = −iħ

Answer: D
A. 0
B. iħ
C. iħ
D. −iħ
E. iħ
(GR0877 #95)
Solution: Commutator identities: [A, B] = − [B, A]
and, [B, AC] = A[B, C] + [B, A]C
[
A =
B =
C =
[
=
=
− [
Answer: D
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